Investigation of mechanical properties of Ruddlesden-Popper 2D,2D-3D and 3D perovskites using an experimental and first principles approach
Hybrid organic-inorganic perovskites (HOIPs) are considered as one of the most promising candidates for the photovoltaic application. Although a lot of research has been done for the improvement in efficiency and stability of the devices made from this material, the mechanical property study of t...
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Format: | Thesis-Doctor of Philosophy |
Language: | English |
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Nanyang Technological University
2023
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Online Access: | https://hdl.handle.net/10356/168825 |
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Institution: | Nanyang Technological University |
Language: | English |
Summary: | Hybrid organic-inorganic perovskites (HOIPs) are considered as one of the most promising
candidates for the photovoltaic application. Although a lot of research has been done for the
improvement in efficiency and stability of the devices made from this material, the mechanical
property study of these materials is very limited. The mechanical properties of hybrid organic inorganic perovskites crystals have been mentioned in a few reports. However, it is also
important to study the mechanical properties of the perovskite’s thin films, especially those
used in flexible devices, since their polycrystalline nature makes them different from single
crystals. The stiffness of the perovskite active layer plays a critical role in influencing the
flexibility of a solar cell. This is one of the important parameters which must be considered
while deciding the architecture of the flexible device. In this study, we report for the very first
time, the elastic modulus of the most commonly used 3D perovskite, i.e., methylammonium
lead iodide (MAPbI3), the pure 2D perovskite (5-AVA)2PbI4 which is based on 5-aminovaleric
acid (5-AVA) cation as well as the 2D-3D mixed perovskites thin films through
nanoindentation technique. The experimental results have also been corroborated by density
functional theory calculations done for the 2D and 3D perovskite. The 2D perovskite shows a
much lower modulus than the 3D perovskite and can be used within a 2D-3D mixture to
improve the mechanical flexibility of the active layer. Also, it is well established that 2D
perovskites are much more stable against moisture as compared to their 3D counterparts due
to the presence of hydrophobic organic alkyl ammonium cation. Thus, the device containing
an active layer comprising a mixture of 3D and 2D perovskite can be used to improve the
environmental stability of the overall device in addition to achieving mechanical durability.
We have also investigated the effect of the number of inorganic layers ‘n’ on the elastic
modulus of 2D, quasi-2D perovskites and 3D perovskite based on butylammonium cation
(BA)2PbI4 and MAPbI3 thin films using nanoindentation technique. Our studies indicate the
role of the orientation of the inorganic layers in perovskite films in tailoring their mechanical
response. The experimental results have been substantiated using first principal density
functional theory (DFT) calculations. We also report other important mechanical parameters,
namely, shear modulus, bulk modulus, Poisson’s ratio, Pugh’s ratio, Vickers hardness, yield
strength and the universal elastic anisotropic index using DFT simulations. Anisotropy is
observed in the elastic modulus of the materials under study and has been discussed in detail
in the manuscript. Understanding the mechanical behavior of 2D Ruddlesden Popper
perovskite thin film in comparison with conventional 3D perovskite offers intriguing insights
into the atomic layer dependent properties and paves the path for next generation
mechanically durable and novel devices.
The present study also includes the measurement of the elastic modulus of the 3D perovskite,
i.e., methylammonium lead iodide (MAPbI3), 2D perovskite, based on phenylethylammonium [(PEA)2PbI4] and mixed 2D-3D perovskite thin film using nanoindentation
technique. First principles density functional theory (DFT) calculations done as part of the
current work on pure 3D and 2D perovskites also corroborate our experimental results. The
effect of the 2D-3D mixture on the elastic modulus has also been investigated, and it has been
found that the modulus values increase with the increase in the percentage of 3D perovskite
within the 2D-3D perovskite mixture. Moreover, a change in the volume fraction of PEA in the
2D-3D mixed perovskite results in a mixture of quasi-2D perovskite in different proportions
within the mixed perovskite. The knowledge gained by comparing DFT and experimental
methodologies allows for the logical design of multilayer HOIPs with mechanical properties
that are suitable for strain-intensive and flexible optoelectronic applications.
In addition to the static mechanical properties, we have also investigated the rate-dependent
inelastic mechanical behaviour in bulk crystals of lead–halide 2D, quasi-2D and 3D perovskites
using nanoindentation creep and stress relaxation measurements at different loading rates.
The mechanical response of these materials to dynamic strain must be understood to
successfully use them in deformable devices. In the current study, a range of perovskites:
CH3NH3PbI3 (3D) perovskite, (BA) butylammonium based 2D perovskite
(CH3(CH2)3NH3)2PbI4, BA based quasi-2D perovskite (CH3(CH2)3NH3)2(CH3NH3)Pb2I7,
(PEA)phenylethylammonium based 2D perovskite (C6H5(CH2)2NH3)2PbI4, and PEA based
quasi-2D perovskite (C6H5(CH2)2NH3)2(CH3NH3)Pb2I7 have been fabricated with particle sizes
ranging in 5-10nm as found using TEM. The nanoindentation creep and stress relaxation
experiments prove the time and rate-dependent mechanical properties of this 2D, quasi-2D,
and 3D HOIPs crystal though varying in their magnitudes. We observe that the 3D, as well as
BA based perovskite samples, show strain rate sensitivity, whereas PEA based perovskite
samples were relatively insensitive towards the rate of loading. Propagation and interaction of
dislocation is much more difficult in PEA-based perovskite, which has a triclinic crystal
structure and is less symmetrical as compared to the BA based perovskite orthorhombic
structure as well as the tetragonal structure of the 3D perovskite. The knowledge offered by
this work is crucial for creating perovskite devices that can endure mechanical deformations. |
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